Lommel function explained

The Lommel differential equation, named after Eugen von Lommel, is an inhomogeneous form of the Bessel differential equation:

z2

d2y
dz2

+z

dy
dz

+(z2-\nu2)y=z\mu+1.

Solutions are given by the Lommel functions sμ,ν(z) and Sμ,ν(z), introduced by,

s\mu,\nu(z)=

\pi
2

\left[Y\nu(z)

z
\int
0

x\muJ\nu(x)dx-J\nu(z)

z
\int
0

x\muY\nu(x)dx\right],

S\mu,\nu(z)=s\mu,\nu(z)+2\mu-1\Gamma\left(

\mu+\nu+1
2

\right)\Gamma\left(

\mu-\nu+1
2

\right) \left(\sin\left[(\mu-\nu)

\pi
2

\right]J\nu(z)-\cos\left[(\mu-\nu)

\pi
2

\right]Y\nu(z)\right),

where Jν(z) is a Bessel function of the first kind and Yν(z) a Bessel function of the second kind.

The s function can also be written as[1]

s\mu,(z)=

z\mu
(\mu-\nu+1)(\mu+\nu+1)

{}1F2(1;

\mu
2

-

\nu
2

+

3
2

,

\mu
2

+

\nu
2

+

3;-
2
z2
4

),

where pFq is a generalized hypergeometric function.

See also

External links

Notes and References

  1. Watson's "Treatise on the Theory of Bessel functions" (1966), Section 10.7, Equation (10)